1989
DOI: 10.1103/revmodphys.61.605
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Thermal boundary resistance

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Cited by 2,594 publications
(2,082 citation statements)
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References 267 publications
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“…Heat transfer at the interface of two different materials mostly happens with a temperature discontinuity [242]. This phenomenon was observed first at the interface of a metal and liquid helium [243], while later it has been found at the interface of two solids [244]. The heat loss at the interface of two different materials is due to the phonon scattering at this region [236,238,239].…”
Section: Thermal Conductivitymentioning
confidence: 96%
“…Heat transfer at the interface of two different materials mostly happens with a temperature discontinuity [242]. This phenomenon was observed first at the interface of a metal and liquid helium [243], while later it has been found at the interface of two solids [244]. The heat loss at the interface of two different materials is due to the phonon scattering at this region [236,238,239].…”
Section: Thermal Conductivitymentioning
confidence: 96%
“…It is reasonable to assume that, for rough interfaces, the scattering becomes diffusive: Carriers lose the memory about their path, and they get scattered in all directions with equal probability. This picture, forming the basis of the ''diffusemismatch model'' of phonon transport, has been employed with success for understanding the thermal conductance of solid-solid interfaces [24][25][26][27]. Thus, it is reasonable to assume a similar diffusive-scattering ansatz for the limiting effect of grain boundaries on charge transport: The carrier mean free path (MFP), , becomes of the order of the grain size, L. For grains smaller than the MFP of the bulk, one can approximate ' L. Contrary to the constantrelaxation-time approximation, this assumption, called the constant-mean-free-path approximation, is based on physical grounds.…”
Section: Introductionmentioning
confidence: 99%
“…4 Such a temperature jump is described by the interface thermal resistance, thermal boundary resistance (TBR), or Kapitza resistance, owing to Kaptiza's original work. 1 With temperature 1 T and 2 T at the two sides of the interface, and heat flux q (W/m 2 ) flowing across the interface, the thermal boundary resistance (R) can be written as,…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3] When phonons transport across a material interface, they experience reflection, transmission, and mode conversion, which results in a local temperature jump at the interface. 4 Such a temperature jump is described by the interface thermal resistance, thermal boundary resistance (TBR), or Kapitza resistance, owing to Kaptiza's original work.…”
Section: Introductionmentioning
confidence: 99%